Giorgio Adamo

Giorgio Adamo


Research Focus & Metrics

Academic Career Length

18Years (2009-Present)

(Calculated once Scilit publication data is synced: current year − year of first publication + 1)

Representative Publications

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28 March 2014 in Nano Letters
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Journal Article
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XDXing Dai
Xing Dai
SZSen Zhang
Sen Zhang
ZWZilong Wang
Zilong Wang
GAGiorgio Adamo
Giorgio Adamo
HLHai Liu
Hai Liu
CSCesare Soci
Cesare Soci

9 September 2009 in Physical Review Letters
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Journal Article
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GAGiorgio Adamo
Giorgio Adamo
KMK. F. MacDonald
K. F. MacDonald
YFY. H. Fu
Y. H. Fu
CWC-M. Wang
C-M. Wang
DTDin Ping Tsai
Din Ping Tsai
NZN. I. Zheludev
N. I. Zheludev
The passage of a free-electron beam through a nanohole in a periodically layered metal-dielectric structure creates a new type of tunable, nanoscale radiation source—a “light well”. In the reported demonstration, tunable light is generated at an intensity of ∼200  W/cm2 as electrons with energies in the 20–40 keV range are injected into gold-silica well structures with a lateral size of just a few hundred nanometers.

2 March 2018 in Science Advances
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Yu ZhouYu Zhou
Yu Zhou
ZWZiyu Wang
Ziyu Wang
ARAbdullah Rasmita
Abdullah Rasmita
SKSejeong Kim
Sejeong Kim
ABAmanuel Berhane
Amanuel Berhane
WGWeibo Gao
Weibo Gao
An optically stable, room temperature single-photon emitter operating in telecom wavelength range is discovered in GaN.

8 October 2014 in Nature Communications
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Journal Article
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Jun-Yu OuJun-Yu Ou
Jun-Yu Ou
JSJin-Kyu So
Jin-Kyu So
GAGiorgio Adamo
Giorgio Adamo
ASAzat Sulaev
Azat Sulaev
LWLan Wang
Lan Wang
NZNikolay I. Zheludev
Nikolay I. Zheludev
The development of metamaterials, data processing circuits and sensors for the visible and ultraviolet parts of the spectrum is hampered by the lack of low-loss media supporting plasmonic excitations. This has driven the intense search for plasmonic materials beyond noble metals. Here we show that the semiconductor Bi1.5Sb0.5Te1.8Se1.2, also known as a topological insulator, is also a good plasmonic material in the blue-ultraviolet range, in addition to the already-investigated terahertz frequency range. Metamaterials fabricated from Bi1.5Sb0.5Te1.8Se1.2 show plasmonic resonances from 350 to 550 nm, while surface gratings exhibit cathodoluminescent peaks from 230 to 1,050 nm. The observed plasmonic response is attributed to the combination of bulk charge carriers from interband transitions and surface charge carriers of the topological insulator. The importance of our result is in the identification of new mechanisms of negative permittivity in semiconductors where visible range plasmonics can be directly integrated with electronics.

5 January 2017 in Advanced Materials
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BGBehrad Gholipour
Behrad Gholipour
GAGiorgio Adamo
Giorgio Adamo
Daniele CortecchiaDaniele Cortecchia
Daniele Cortecchia
HKHarish N. S. Krishnamoorthy
Harish N. S. Krishnamoorthy
Muhammad Danang BirowosutoMuhammad Danang Birowosuto
Muhammad Danang Birowosuto
CSCesare Soci
Cesare Soci

23 March 2022 in Nature Communications
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GLGuankui Long
Guankui Long
GAGiorgio Adamo
Giorgio Adamo
JTJingyi Tian
Jingyi Tian
MKMaciej Klein
Maciej Klein
HKHarish N. S. Krishnamoorthy
Harish N. S. Krishnamoorthy
CSCesare Soci
Cesare Soci
Recent attempts to synthesize hybrid perovskites with large chirality have been hampered by large size mismatch and weak interaction between their structure and the wavelength of light. Here we adopt a planar nanostructure design to overcome these limitations and realize all-dielectric perovskite metasurfaces with giant superstructural chirality. We identify a direct spectral correspondence between the near- and the far- field chirality, and tune the electric and magnetic multipole moments of the resonant chiral metamolecules to obtain large anisotropy factor of 0.49 and circular dichroism of 6350 mdeg. Simulations show that larger area metasurfaces could yield even higher optical activity, approaching the theoretical limits. Our results clearly demonstrate the advantages of nanostructrure engineering for the implementation of perovskite chiral photonic, optoelectronic, and spintronic devices.